To solve this problem, we need to apply the principle of conservation of momentum. The total momentum before and after the breakup of the object must be equal.
Let's denote:
The total mass of the original object is divided into two parts with a mass ratio of 1:5.
If the smaller mass is m, the larger mass will be 5m.
According to the conservation of momentum:
\( (m + 5m)\vec{V}_i = m\vec{V}_s + 5m\vec{V}_l \)
Since the total mass cancels out from both sides, we can simplify to:
\(\vec{V}_i = \frac{1}{6} \left(\vec{V}_s + 5\vec{V}_l\right) \)
Substituting the known values, we get:
\((20\hat{i} + 25\hat{j} - 12\hat{k}) = \frac{1}{6}\left((100\hat{i} + 35\hat{j} + 8\hat{k}) + 5\vec{V}_l\right)\)
Rearranging for \(\vec{V}_l\):
\(6(20\hat{i} + 25\hat{j} - 12\hat{k}) = (100\hat{i} + 35\hat{j} + 8\hat{k}) + 5\vec{V}_l\)
\((120\hat{i} + 150\hat{j} - 72\hat{k}) - (100\hat{i} + 35\hat{j} + 8\hat{k}) = 5\vec{V}_l\)
\(20\hat{i} + 115\hat{j} - 80\hat{k} = 5\vec{V}_l\)
Now, divide by 5 to solve for \(\vec{V}_l\):
\(\vec{V}_l = \frac{1}{5}(20\hat{i} + 115\hat{j} - 80\hat{k})\)
\(\vec{V}_l = 4\hat{i} + 23\hat{j} - 16\hat{k}\)
Therefore, the velocity of the larger piece is \(\boxed{4\hat{i} + 23\hat{j} - 16\hat{k}}\), which matches the correct option given.